平面 p 和 q 的方程分别为: r=(2+λ−2μ) i+(−3λ+μ) j+(3−λ+2μ) kr = (2 + \lambda - 2\mu)\,\mathbf{i} + (-3\lambda + \mu)\,\mathbf{j} + (3 - \lambda + 2\mu)\,\mathbf{k} 与 r⋅(a−1b)=1r \cdot \begin{pmatrix} a \\ -1 \\ b \end{pmatrix} = 1, 其中 a 和 b 是常数,λ\lambda 和 μ\mu 是参数。 直线 l 通过点 (5,4,0) 且平行于向量 −2i−j+2k-2\mathbf{i} - \mathbf{j} + 2\mathbf{k}。平面 p 和 q 相交于直线 l。

  1. (a)

    证明 a=1a = 1 且 b=12b = \tfrac{1}{2}。

  2. (b)

    求平面 p 和 q 之间夹角的锐角精确值。

  3. (c)

    求点 A(2,0,3) 到平面 q 的距离。由此推导点 A 到直线 l 的最短距离。

  4. (d)

    平面 q 关于平面 p 镜面反射得到平面 q'。

    求平面 q' 的笛卡尔方程。

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完整解法

9(a)

1. Substitute the position vector of the known point on $l$ into the equation of plane $q$ to find $a$.

Since the line ll lies on the plane qq, any point on ll must satisfy the equation of qq. We are given that ll passes through (5,4,0)(5, 4, 0).
(540)⋅(a−1b)=1\begin{pmatrix} 5 \\ 4 \\ 0 \end{pmatrix} \cdot \begin{pmatrix} a \\ -1 \\ b \end{pmatrix} = 1
5(a)+4(−1)+0(b)=15(a) + 4(-1) + 0(b) = 1
5a−4=15a - 4 = 1
5a=5  ⟹  a=15a = 5 \implies a = 1

2. Use the condition that the direction vector of $l$ is perpendicular to the normal vector of $q$ to find $b$.

Since the line ll is entirely on the plane qq, its direction vector must be perpendicular to the normal vector of qq. Thus, their scalar product is zero.
(−2−12)⋅(1−1b)=0\begin{pmatrix} -2 \\ -1 \\ 2 \end{pmatrix} \cdot \begin{pmatrix} 1 \\ -1 \\ b \end{pmatrix} = 0
−2(1)+(−1)(−1)+2(b)=0-2(1) + (-1)(-1) + 2(b) = 0
−2+1+2b=0-2 + 1 + 2b = 0
2b−1=0  ⟹  2b=1  ⟹  b=122b - 1 = 0 \implies 2b = 1 \implies b = \frac{1}{2}

答案

a = 1 \text{ and } b = \frac{1}{2} \text{ (shown)}

9(b)

1. Find the normal vector to plane $p$.

From the parametric equation of plane pp, the two direction vectors are d1=(1−3−1)\mathbf{d}_1 = \begin{pmatrix} 1 \\ -3 \\ -1 \end{pmatrix} and d2=(−212)\mathbf{d}_2 = \begin{pmatrix} -2 \\ 1 \\ 2 \end{pmatrix}.
The normal vector to plane pp is their cross product:
np=(1−3−1)×(−212)=((−3)(2)−(−1)(1)(−1)(−2)−(1)(2)(1)(1)−(−3)(−2))=(−50−5)\mathbf{n}_p = \begin{pmatrix} 1 \\ -3 \\ -1 \end{pmatrix} \times \begin{pmatrix} -2 \\ 1 \\ 2 \end{pmatrix} = \begin{pmatrix} (-3)(2) - (-1)(1) \\ (-1)(-2) - (1)(2) \\ (1)(1) - (-3)(-2) \end{pmatrix} = \begin{pmatrix} -5 \\ 0 \\ -5 \end{pmatrix}
For simpler calculations, we can take a parallel vector np=(101)\mathbf{n}_p = \begin{pmatrix} 1 \\ 0 \\ 1 \end{pmatrix}.

2. Identify the normal vector to plane $q$.

Using a=1a = 1 and b=12b = \frac{1}{2} from part (a), the equation of plane qq is r⋅(1−112)=1\mathbf{r} \cdot \begin{pmatrix} 1 \\ -1 \\ \frac{1}{2} \end{pmatrix} = 1.
The normal vector to plane qq is:
nq=(1−112)\mathbf{n}_q = \begin{pmatrix} 1 \\ -1 \\ \frac{1}{2} \end{pmatrix}
To avoid fractions, we can take a parallel vector nq=(2−21)\mathbf{n}_q = \begin{pmatrix} 2 \\ -2 \\ 1 \end{pmatrix}.

3. Calculate the exact acute angle between the planes.

Let θ\theta be the acute angle between the planes, which corresponds to the acute angle between their normal vectors.
cos⁡θ=∣np⋅nq∣∣np∣∣nq∣=∣(101)⋅(2−21)∣12+02+1222+(−2)2+12\cos \theta = \frac{|\mathbf{n}_p \cdot \mathbf{n}_q|}{|\mathbf{n}_p| |\mathbf{n}_q|} = \frac{\left| \begin{pmatrix} 1 \\ 0 \\ 1 \end{pmatrix} \cdot \begin{pmatrix} 2 \\ -2 \\ 1 \end{pmatrix} \right|}{\sqrt{1^2+0^2+1^2} \sqrt{2^2+(-2)^2+1^2}}
cos⁡θ=∣2+0+1∣29=332=12\cos \theta = \frac{|2 + 0 + 1|}{\sqrt{2} \sqrt{9}} = \frac{3}{3\sqrt{2}} = \frac{1}{\sqrt{2}}
Since we need the exact acute angle,
θ=π4 (or 45∘)\theta = \frac{\pi}{4} \text{ (or } 45^\circ)

答案

π4\frac{\pi}{4} (or 45∘45^\circ)

9(c)

1. Find the perpendicular distance from point A to plane q.

From part (a), a=1a=1 and b=12b=\frac{1}{2}. The equation of plane q is r⋅(1−11/2)=1\mathbf{r} \cdot \begin{pmatrix} 1 \\ -1 \\ 1/2 \end{pmatrix} = 1, which can be scaled to r⋅(2−21)=2\mathbf{r} \cdot \begin{pmatrix} 2 \\ -2 \\ 1 \end{pmatrix} = 2.

The perpendicular distance from A(2,0,3)A(2, 0, 3) to plane q is:
AM=∣2(2)+(−2)(0)+1(3)−2∣22+(−2)2+12AM = \frac{|2(2) + (-2)(0) + 1(3) - 2|}{\sqrt{2^2 + (-2)^2 + 1^2}}
AM=∣4+0+3−2∣9=53AM = \frac{|4 + 0 + 3 - 2|}{\sqrt{9}} = \frac{5}{3}

2. Concisely evaluate the acute angle between planes p and q (result from part b).

The normal to plane p is np=(1−3−1)×(−212)=(−50−5)\mathbf{n}_p = \begin{pmatrix} 1 \\ -3 \\ -1 \end{pmatrix} \times \begin{pmatrix} -2 \\ 1 \\ 2 \end{pmatrix} = \begin{pmatrix} -5 \\ 0 \\ -5 \end{pmatrix}.
The normal to plane q is nq=(2−21)\mathbf{n}_q = \begin{pmatrix} 2 \\ -2 \\ 1 \end{pmatrix}.
If θ\theta is the acute angle between the planes:
cos⁡θ=∣np⋅nq∣∣np∣∣nq∣=∣−10+0−5∣509=15152=12\cos \theta = \frac{|\mathbf{n}_p \cdot \mathbf{n}_q|}{|\mathbf{n}_p| |\mathbf{n}_q|} = \frac{|-10 + 0 - 5|}{\sqrt{50} \sqrt{9}} = \frac{15}{15\sqrt{2}} = \frac{1}{\sqrt{2}}
θ=45∘\theta = 45^\circ

3. Use geometric reasoning to deduce the shortest distance from A to l.

By substituting λ=0\lambda = 0 and μ=0\mu = 0 into the equation of plane p, we obtain the position vector (203)\begin{pmatrix} 2 \\ 0 \\ 3 \end{pmatrix}, confirming that A lies exactly on plane p.
Line ll is the intersection of planes p and q, so it lies on both planes.
Let MM be the foot of the perpendicular from A to q, and NN be the foot of the perpendicular from A to ll.
Since ll lies on q and AM⊥qAM \perp q, we have AM⊥lAM \perp l. By definition, AN⊥lAN \perp l.
Thus, ll is perpendicular to the plane AMNAMN. This means ∠ANM\angle ANM corresponds exactly to the acute angle between planes p and q, so ∠ANM=45∘\angle ANM = 45^\circ.
In the right-angled △AMN\triangle AMN:
sin⁡45∘=AMAN  ⟹  AN=AMsin⁡45∘=5/31/2=523\sin 45^\circ = \frac{AM}{AN} \implies AN = \frac{AM}{\sin 45^\circ} = \frac{5/3}{1/\sqrt{2}} = \frac{5\sqrt{2}}{3}
The shortest distance from A to ll is 523\frac{5\sqrt{2}}{3}.

答案

Distance to plane q is 53\frac{5}{3}.
Shortest distance to ll is 523\frac{5\sqrt{2}}{3}.

9(d)

1. Deduce the geometric relationship and angle between plane $q$ and its reflection $q'$.

From part (b), the acute angle between the mirror plane pp and plane qq is 45∘45^\circ.
Since plane q′q' is the reflection of qq about pp, the angle between qq and q′q' is 2×45∘=90∘2 \times 45^\circ = 90^\circ.
Thus, plane q′q' is perpendicular to plane qq.

2. Find the normal vector of plane $q'$ using the cross product.

Since q′⊥qq' \perp q, its normal vector nq′\mathbf{n}_{q'} is perpendicular to the normal vector of qq, nq=(2−21)\mathbf{n}_q = \begin{pmatrix} 2 \\ -2 \\ 1 \end{pmatrix}.
Plane q′q' also contains the intersection line ll, so nq′\mathbf{n}_{q'} must be perpendicular to the direction vector of ll, dl=(−2−12)\mathbf{d}_l = \begin{pmatrix} -2 \\ -1 \\ 2 \end{pmatrix}.
We find nq′\mathbf{n}_{q'} using the cross product:
nq′=nq×dl=(2−21)×(−2−12)=(−4−(−1)−2−4−2−4)=(−3−6−6)\mathbf{n}_{q'} = \mathbf{n}_q \times \mathbf{d}_l = \begin{pmatrix} 2 \\ -2 \\ 1 \end{pmatrix} \times \begin{pmatrix} -2 \\ -1 \\ 2 \end{pmatrix} = \begin{pmatrix} -4 - (-1) \\ -2 - 4 \\ -2 - 4 \end{pmatrix} = \begin{pmatrix} -3 \\ -6 \\ -6 \end{pmatrix}
We can scale this to get a simpler parallel normal vector: n=(122)\mathbf{n} = \begin{pmatrix} 1 \\ 2 \\ 2 \end{pmatrix}.

3. Form the cartesian equation of plane $q'$ using a point on the plane.

The line ll passes through the point (5,4,0)(5, 4, 0), which must therefore lie on plane q′q'.
Using the scalar product equation of a plane r⋅n=a⋅n\mathbf{r} \cdot \mathbf{n} = \mathbf{a} \cdot \mathbf{n}:
r⋅(122)=(540)⋅(122)\mathbf{r} \cdot \begin{pmatrix} 1 \\ 2 \\ 2 \end{pmatrix} = \begin{pmatrix} 5 \\ 4 \\ 0 \end{pmatrix} \cdot \begin{pmatrix} 1 \\ 2 \\ 2 \end{pmatrix}
r⋅(122)=5(1)+4(2)+0=13\mathbf{r} \cdot \begin{pmatrix} 1 \\ 2 \\ 2 \end{pmatrix} = 5(1) + 4(2) + 0 = 13
The cartesian equation of the plane q′q' is:
x+2y+2z=13x + 2y + 2z = 13

答案

x+2y+2z=13x + 2y + 2z = 13

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